Research Article Volume 4 Issue 4
Structural department, Faculty of Engineering, Ain Shams University, Egypt
Correspondence: Judy MI Soliman, Assistant Professor, Structural department, Faculty of Engineering, Ain Shams University, 35 West Golf Area, 5th Settlement, New Cairo, Cairo, Egypt, Tel 2 0100 5455 580
Received: June 18, 2017 | Published: July 23, 2018
Citation: Soliman JMI. General behavior of t- section RC beams strengthened with epoxy-bonded carbon strands. MOJ Civil Eng. 2018;4(4):213-217. DOI: 10.15406/mojce.2018.04.00121
There are no widely accepted guidelines for the design of concrete girders strengthened in shear using externally bonded FRP systems. The current research introduces the use of externally bonded CFRP strands to strengthen the beams in shear and increase its shear capacity, not in a U–shape form, but in a discrete form– on the sides only. Experimental behavior and test results of five T–section RC beams strengthened in shear are present. The main objectives of this research are to evaluate, based on the experimental work, the impact of CFRP strands amount per strip and spacing between strips on the shear behavior of RC beams and to evaluate the applicability of existing analytical models of RC beams strengthened in shear with CFRP Strands. The discrete strips of CFRP Strands are applied with different widths and spacing, bonded externally to the test specimens in order to observe the overall behavior of the RC T–beams and the mode of failure of the applied Carbon Strands strips. Results from the experimental program shows that the application of Carbon Strands strips to RC T–beams did in fact enhance the overall behavior of the specimens. The strengthened specimens respond with an increase in shear capacity. The spacing between the CFRP strands should be less than half the effective depth of the strengthened beam (d/2), and larger than the sum of width of the strengthening strip and the quarter of the effective depth of the specimen (W+d/4). The geometry of the CFRP strands allows full penetration of the epoxy through the strengthening strips, which eliminates the deboning of the strips. The dominant mode of failure is cracking of the concrete cover under the CFRP strands strips, separating the strengthening strips from the specimens, followed by shear failure.
Keywords: shear, externally bonded, FRP, strengthening, RC beam, carbon strands, epoxy
CS; Carbon Strands Sheet, FRP; Fiber Reinforced Polymers, fy: yield strength of steel bars, d: beam effective depth, ts: slab thickness, tb: beam total thickness, B: flange width, b: web width, W: width of the strengthening CFRP strands strip
In recent years, repair and retrofit of existing structures with externally bonded FRPs have been among the most important challenges in civil engineering. The need to strengthen and rehabilitate existing concrete and steel structures has increased the use of fiber reinforced polymers (FRP) in structural strengthening applications since the mid 1980’s.1 Although it is demonstrated by many researchers and practitioners that FRP systems have significant potential for various civil engineering applications, they mostly rally to become the prime material among the other alternatives for retrofit and rehabilitation of the reinforced concrete structures. Such FRP systems are lightweight, exhibit high tensile strength, are not prone to electrochemical corrosion, they can be formed, fabricated, are easy to install, and bonded easily to concrete substrate; these features facilitate handling and help expedite repair or construction. The high strength– to–weight ratio of FRP composites makes them more structurally efficient than traditional strengthening materials.2 Extensive research has shown that FRP systems improve both short and long term flexural behavior of concrete girders. Externally bonded FRP systems composites are generally used for flexural strengthening, confinement and improvement of ductility in columns, or shear strengthening. Although the flexural strengthening is the main dominant on the use of FRP, in such cases, the shear capacity should be enhanced to avoid catastrophic failures. A significant amount of research has been conducted on flexural and axial strengthening but limited investigations have been conducted on the use of externally bonded FRP for shear strengthening. Several analytical studies have dealt with the shear behavior of concrete girders strengthened with FRP systems and a number of models were developed to predict such behavior and found that the size–effect of test specimens has little influence on the effectiveness of externally bonded FRP and thus empirical design expressions calibrated from small– scale test results should provide reasonable accuracy.3 However, the analytical and experimental studies on shear strengthening with FRP systems are limited. Nevertheless, some of these studies have shown that FRP systems can provide an effective means for increasing the shear capacity of concrete girders; still, there are no widely accepted guidelines for the design of concrete girders strengthened in shear using externally bonded FRP systems.
In this research, an experimental program is devised to investigate the shear resistance of Carbon Strands externally bonded to RC T–section beams. No experimental tests have been conducted on beams shear– strengthened with Carbon Strands externally bonded on the sides only in II– shape not U– shaped shear– strengthening. All experimental beams are specially designed to fail in shear in order to better study the interaction between the concrete and the externally applied Carbon Strands. The general goal of this research is to study the shear behavior of RC T–beams strengthened with Carbon strands on the beams sides only. Aiming at this goal, five RC T–beams are designed such that a shear failure is induced to the beams. The test specimens in this experimental study are strengthened with external strips of II– shape Carbon Strands at different spacing, it should be noted that the CFRP strips are not effective at all at spacing greater than half the effective depth of the specimen.4 Previous researches investigated the two–sided wrapping in shear strengthening and advised that either wrap all schemes continuously or discretely,5 concluded that center to center spacing between strips must be equal or smaller than (d/4+strip width). It is hypothesized that strengthening the RC T–beams with Carbon Strands increases the overall shear capacity of the beams.
Concrete mix: All beams are cast from the same concrete mix which has a 28 day mean compressive cylinder strength of 40 N/mm2. The mix consists of type I cement with maximum limestone coarse aggregate sizes of 19 mm and 13 mm.
Longitudinal Steel Reinforcement of High Tensile steel (fy: 360 N/mm2): each beam is reinforced in flexure with 6 bars of 25 mm diameter on 3 rows, spaced with a 25 mm transverse separator. The top flange is reinforced using 4 longitudinal steel bars with 12mm. diameter, and 6mm diameter bars in the transverse direction, as shown in Figure 2A.
Transverse reinforcement of Mild steel (fy: 240 N/mm2): closed stirrups of 8 mm. diameter are distributed along the beams with spacing of 170 mm, as d/2=168 mm.
Strengthening sheets: Carbon Strands Sheets (Figure 1), Japanese sheets: Tensile strength: 2060 N/mm2, Modulus of Elasticity: 118 GPa, and Ultimate strain of 0.0175. It is a unidirectional carbon strand, each strand of 0.572 mm. diameters, they come attached together in sheets of dimensions 500 × 3000 mm.
Epoxy: adhesive material: Chimapoxy 2000, Egyptian Product, manufactured by CMB Group. The Chimapoxy had a pot life of 3 hours, a working time of 30 to 60 minutes and a cure time of 24 hours. All test specimens had cured at least 7 days before being placed on the reaction frame for shear testing. (Figure 2).
Beams specimens
Strengthening schema
Beam ID |
CS strip width “W” mm. |
CS strips spacing mm. |
Bo |
N/A |
N/A |
B3II10 |
30 |
100 |
B3II17 |
30 |
170 |
B5II15 |
50 |
150 |
B5II17 |
50 |
170 |
Table 1 Test matrix
All five test specimens are subjected to a three point loading system and failed as expected in a shear failure. Shear cracks are marked as they appear on the specimen along with the corresponding load during the test. Figure 3 shows the load versus mid–span deflection relations of the tested beams. Typical load deflection behavior comparing the control beam Bo to the strengthened beams reflecting the effect of the strengthening strips width between B3II17 AND B5II17, and the effect of center line to center line spacing between strips by comparing B3II10 with B3II17, and B5II15 with B5II17. Test results indicate that the pre and post cracking stiffness are identical for B5II15 and B5II17 which experienced a brittle shear failure, without neither warning nor moderate shear cracks propagation, and subjected to a 3% decrease in the load carrying capacity in B5II15, as for B5II17. Using thin CS strips in B3II10 and B3II17 allows shear cracks propagation through the beam prior to failure; hence lead the strengthened beams to exert a ductile failure. The beams experienced an increase in the load carrying capacity of 10 %, and 22% for B3II10, and B3II17, respectively.
Figure 4 shows the vertical displacement profile of the control beam, where the data from two LVDTs on both sides of the beam are shown to be similar, and hence more reliable. The largest shear cracks are noticed at the south end of all tested specimens where the loss of aggregate interlock occurred at failure. The control beam failed in shear with shear cracks propagating from the support to the top flange at an approximately 45° angle. Figure 5 shows the failure pattern and the location of the shear cracks at failure of Bo, under ultimate load of 470.83 kN. The largest vertical deflection was measured by LVDT located at the midsection of the beam, and was 10.38 mm. As expected, the control beam failed in a brittle manner. The presence of the CS strips of width 50 mm. strengthening beams B5II15, and B5II17, also led to a brittle failure, where the shear cracks propagate with 45° angle, from the third strip approximately at distance d from support, to the top flange. Figure 6 & Figure 7 show the failure pattern and the location of the shear cracks at failure, under ultimate loads of 455.72, and 481.48 kN, respectively. The largest vertical deflection are measured by LVDT located at the midsection of the beams, and are 9.62, and 9.39 mm. respectively. Specimens B3II10 and B3II17 failed as expected in shear, showing diagonal shear cracks that initiate from the supports up to the loading point and through the CS strips ((Figure 8) (Figure 9) respectively). The largest shear crack is located at the south end of the beam in the shear span area. The ultimate loads carried by the strengthened beams are 519.8, and 577.35 kN, respectively. Upon failure, the concrete cover cracked under the CS strips, fully separating the strips or partially separated from the specimens, bridging the shear cracks leading to failure. The maximum vertical deflection is also measured by LVDT, where the larger deflection is noted on the failed zone for tested beams as illustrated in Table 2. The tensile strains in the transverse reinforcements (stirrups) were measured with steel strain gauges and shown in Figure 10 & Figure 11. The control beam exerted brittle failure due to crack propagation from support to top flange with angle 45o, no sudden jumps in the strain gauges reading are illustrated as Bo failed due to crushing of concrete at support location. For beams B5II15 and B5II17, they failed suddenly at loads close to the failure load of the control beam. The sudden jump in the strain gauges is caused by the shear cracks at angle 45o. Beam B3II17 was able to carry more load than the control beam Bo. The strain gauges reading varied appropriately with the increase in the load, hence the shear carrying capacity of the beam increased. The sudden jump in strain reading at angle 45o was detected after failure, the reading of tensile strain at crack propagation was not recorded due to error in the strain gauge reading, as shown in Figure 11, and constant strain reading was recorded for a wide range of loading. As for B3II10, the shear cracks propagated in the two directions, 45o from support to top flange, and the support to loading point, the critical shear crack is from the support to loading point, which is illustrated by the uniform increase in the tensile strain readings of B3II10 on the 45o crack angle from the support in Figure 10 and the sudden jump in the strain readings of B3II10 on the crack from support to loading point in Figure 11.
Beam ID |
Failure load (kN) |
Maximum deflection at |
Maximum deflection at |
Maximum tensile strain |
Maximum tensile strain |
Bo |
470.83 |
10.38 |
8.18 |
2035 |
9772 |
B3II10 |
519.8 |
9.73 |
9.32 |
9162 |
2598 |
B3II17 |
577.35 |
10.33 |
10.03 |
6268 |
11677 |
B5II15 |
455.72 |
9.62 |
9.66 |
11424 |
1490 |
B5II17 |
481.48 |
9.39 |
9.79 |
10866 |
9943 |
Table 2 Summary of experimental results
My sincere gratitude to North Carolina State University for supplying the Carbon Strands sheets used in this research work. Many thanks are extended to the entire staff at the Structural Laboratory of Ain Shams University for their help with all aspects of this project.
The author declares there is no conflict of interest.
©2018 Soliman. This is an open access article distributed under the terms of the, which permits unrestricted use, distribution, and build upon your work non-commercially.