Figure 9 illustrates the relation between torsional moments and angles of twist and Fig. 10 represents the crack pattern of the tested beams. In this comparison, it was shown that the results of the first control box girder CB1 are very close to that of the second control one CB2, whether in terms of the angle of rotation or the value of resistance to torsion. For the control specimen that had an opening, the value of the maximum torsion was decreased by about 39% compared to the CB1. The solid beam showed the highest value of torque resistance. The maximum load of this beam was 213.49 kN which resulted in a torsional torque of 43.76 kN.m at a twisting angle of 0.0149 rad/m. Then the load suddenly decreased from 225 kN to 76 kN. The solid beam has the ability to demonstrate the torsion torque by a greater percentage than the box beams up to a 50% percentage. The maximum load of the control beam was 142.63 kN which causes a torsional torque of 29.24 kN.m at an angle of twist 0.0107 rad/m. The maximum load of the beam with opening reached 87.16 kN and caused torsional torque of 17.87 kN.m and an angle of rotation of 0.0054 rad/m as shown in Fig. 9. In this sample, a collapse occurred at a lower value than the control specimens due to the presence of the opening. The presence of the aperture caused the sample to lose 39% of the torsional resistance, compared to the control box girder without an opening.
From Fig. 10, it can be seen that for solid beam, some cracks extended under the loading frame until crushed were occurred and a part of the concrete crushed until it reached the reinforcing main steel. The size of the crack caused was within 4 mm. In the test of the control box beam, one crack occurred until it reached the steel rebar. The crack was diagonally at an angle of around 45 degrees and it extended until it reached the bottom of the loading frame. There were some slight cracks around the main crack with the same angle of inclination. The main crack almost occurred in the middle of the face, facing the load. The main crack extended in the form of a V shape at two faces of the specimen. For CBO, at first, one crack occurred around the specimen, and with increasing load, the cracks increased around the opening. The crack size was about 1.0 mm on the opposite side when taking readings. A portion of the concrete around the opening was crushed as shown in Fig. 10. In Fig. 10, comparing box girders containing openings with (BOS and BOF specimens) and without strengthening (CBO specimen) through the relationship between torsion and twisting angle, which shows that strengthened specimens’ failure torque was obtained with a value close to the failure value of the control specimen CB1. This indicates the efficiency of the strengthening in restoring the reduction of torsional stiffness due to the opening. In addition, the collapse of specimen BOF was a result of the separation of the fiber. The beam with steel strip: BOS reached 141.19 kN ultimate load and caused 28.94 kN.m torsional moment of and 0.0088 rad/m twisting angle. The maximum load of BOF was 114.1 kN at a torsional torque of 23.39 kN.m and a twisting angle of 0.0105 rad/m. Cracks occurred around the opening in the two beams BOS and BOF which were strengthened by steel and CFRP, respectively, as an angle of inclination of 45 degrees and it started at the end of the strengthening strips as shown in Fig. 10. Due to the use of a resin material and the anchor bolts, a higher control and resistance to cracks occurred. The size of the cracks in BOS was about 0.85 mm around the hole. On the other hand a de-bonding and separation of the CFRP strips was observed at the end of the test of the BOF specimen. The size of the cracks around the opening is approximately 1.6 mm for BOF.
Figure 9 represents the relationship between the torsional moment and the twisting angle for comparison between the control specimen (CB1) and the strengthened box girders, whether with longitudinal or U-shaped steel strips of 1 mm thickness: beams of group (3). The use of longitudinal strengthening resisted the propagation of cracks, which led to a reduction in the bitch and led to a change in the direction of the cracks laterally as shown Fig. 10 and it was in the range of 1.1 mm. Steel strips resisted the occurrence of adjacent cracks and pitch of the BUS specimen that was strengthened with steel plates as U-shaped as shown in Fig. 10. The size of the crack at the opposite side of the load was about 5.0 mm and no separation of steel strips from the concrete was observed. It was found that the torsional resistances increased by values of 32% and 16% in the strengthened specimens in a longitudinal and U-shaped, respectively.
Figure 9 shows the comparison between the control specimen and box girders strengthened with CFRP as a relationship between the torsional moments versus the twisting angle. It is shown that the box girder strengthened by longitudinal or longitudinal with U-shaped strips has better behavior than strengthened with only U-shaped strips. The maximum load was 170.50 kN at a twisting angle of 0.0128 rad/m and the maximum torsion torque was 34.95 kN.m. The use of longitudinal sheets of CF led to an increase in the number of cracks and it did not allow cracks to continue as plotted in Fig. 10. The bond between the concrete and the fiber was good even after the collapse so that a separation was taken place for only one strip. A concentration of stress occurred at the bottom of the loading frame, and this coincided with the separation of the fiber strip. Also, cracks occurred on the face that was not strengthened with the carbon fiber due to the resistance of the fiber in the other sides. The size of the crack at the destination corresponding to the loading was 0.45 mm. For specimen BUF, which was strengthened with U-shaped form, the fiber slice was separated from the reinforced concrete as shown in Fig. 10. The separation of the fiber strips led to a single crack, and its width increased by increasing loads. on the opposite sides of taking readings, the fibers resisted the continuation of the crack and therefore their number increased, and this also occurred in the strengthened lower face. By measuring the width of the cracks on the side opposite the readings, it was from 0.3 mm to 0.9 mm. The highest load was 185.42 kN at a twisting angle of 0.0073 rad/m and torsional torque 38.01 kN.m.
The maximum load of the BLUF sample was 212.23 kN producing a torque of 43.51 kN.m and a twisting angle of 0.0231 rad/m as shown in Fig. 9. After reaching the ultimate load, the load decreased by small values by increasing the angle of rotation. The sample loading process was stopped and did not continued until the load reached significantly lower values, where a large rotation angle occurred, and there was a fear that the sample fell due to the occurrence of rotations from one direction to the other direction. The presence of fiber strips in both directions on the three sides of the specimen led to a higher control. It also led to an increase in cracks in the un-strengthened face, which includes a large crack as shown in Fig. 10. A separation occurred between the bonding material of the fiber and the concrete for a small part in the top layer corresponding to the un-strengthened face, and this occurred as a result of the widening of the crack. The size of the cracks ranged from 0.25 mm to 1.0 mm.
Figure 11 and Fig. 12 compare the control specimens and the strengthened box girders by U-shaped and longitudinal strips, whether steel or CFRP, respectively. It is shown that torsional moment values were obtained with lower rotation angle values compared with the values of the reference specimens and the retrofitted box girders provided higher torsional resistance than the control specimens. Also, applying longitudinal steel strips gave higher structural performance for BGs than FRP Strips under torsional loads.
Figure 13 plots the relevance between the angle of rotation and the torsional moment of specimens as a comparison between the numerical (NU) and experimental (EX) results. This figure presents that the CB1 specimen remained in the elastic phase until the value of the torsional moment for EX results was equal to 26.5 kN.m and the value equal to 25 kN.m for NU. In this part, EX results were very close to NU results. After that, the sample moved to the phase of plasticity in which the sample reached the ultimate torsional moment equal to 28.10 kN.m with a twisting angle = 0.01171 rad/m for NU result and for EX result equals 29.24 kN.m with a twisting angle equals to 0.01072 rad/m. The value of the ultimate torsional moment in NU is less than the EX by 3.9%. After reaching the ultimate stage, the value of the torsional moment begins to decrease as the value of the angle of rotation increases until the collapse occurs. Figure 14 shows the crack pattern for FEM results, which shows a high level of agreement with experimental findings. Significantly the same results when comparing the second experimental specimen CB2 results with FEM. The comparison revealed that the experimental and FEM results were in good agreement.
The CBO specimen remained in the elastic phase until the EX torsion moment reached 15 kN.m and the NU torsion moment reached 13.8 kN.m, as plotted in Fig. 13. The practice and NU outcomes were fairly similar in this section. The sample next entered the plasticity phase, where it reached an ultimate torsional moment that was equal to 17.66 kN.m at a twisting angle of 0.01200 rad/m as the NU result and 17.87 kN.m at a twisting angle of 0.00544 rad/m as the EX result. The ultimate torsional moment from the NU was lower than the EX results by 1.2%. After reaching the last stage, the torsional moment starts to decrease as the angle of rotation increases, until the specimen collapses. Figure 14 shows the experimental and FEM crack patterns. The solid beam is one of the tested beams in group 1 as control beams. The angle of rotation versus the torsional moment curves of CS is shown in Fig. 13. The specimen remained in the elastic phase until the torsional moment was equivalent to 41.5 kN.m as the EX results and 37.5 kN.m in the NU. The EX and NU results were extremely similar in this section. The sample then entered the phase of plasticity, where it reached an ultimate torsional moment of 41.77 kN.m with a twist angle of 0.01400 rad/m from the NU curve, and 43.76 kN.m with a twist angle of 0.01065 rad/m from the EX curve. The NU value of the torsional moment is less by 4.5 percent than the EX value in this stage. The crack pattern for this specimen from the EX and NU is closed and it was not listed to prevent elongation.
Group (2) contains the box girders with an opening, which were strengthened by applying the strengthening material around the opening. It consists of two specimens; BOS and BOF. The first box girder was strengthened with CFRP and the second box girder was strengthened with steel plate strips. The relationship between the angle of rotation and the torsional moment of BOS and BOF is shown in Fig. 13. The specimen remained in the elastic phase until the torsion moment was equal to 25 kN.m for EX and equal to 28 kN.m for NU. The NU results were fairly close to the experimental results in this section. After that, the sample started the phase of plasticity, where it attained 35.77 kN.m an ultimate torsional moment with 0.01143 rad/m a corresponding angle of rotation from NU curve, and 28.94 kN.m with a rotation angle of 0.00884 rad/m from the EX curve. The Numerical results are greater by 23.6% than the EX in this stage. After reaching the last stage of loading, the torsional moment begins to reduce as the angle of rotation increases, until the girder collapses. The BOF sample remained in the elastic phase until the torsional moment for the EX results was equal to 20.5 kN.m and equal to 18 kN.m for NU, as shown in Fig. 13. Then, the plasticity stage was begun, where it lasted until the ultimate torsional moment reached 24.32 kN.m at a twisting angle of 0.01343 rad/m as NU, and 23.39 kN.m at a twisting angle of 0.01051 rad/m as the EX results. The NU results of this sample were fairly close to the EX results. The crack pattern of the specimens of this group from the EX and NU is closed that it simulated as a concentrated crack round the opening and it was sufficient to list one sample; BOF, as an example in Fig. 14 to prevent elongation.
In group (3), the results of box girders strengthened with steel plate strips are reviewed. The set consists of two girders, one of which was strengthened with longitudinal steel strips (BLS) and the other was strengthened with U-shaped steel strips (BUS). Figure 13 plots the relevance between the angle of rotation and the torsional moment of BLS. This figure shows that the sample remained in the elastic phase until the value of the torsion moments for EX and NU were approximately 37 kN.m. After that, the sample moved to the phase of plasticity in which the sample reached the ultimate torsional moments equal 42.76 kN.m and 38.69 kN.m with corresponding 0.00914 rad/m and 0.01167 rad/m angles of rotation for NU and EX outputs, respectively. The value of the torsional moment of the NU is more than the EX by 10.5%. After reaching the ultimate stage, the value of the torsional moment begins to decrease as the value of the angle of rotation increases until the collapse occurs. For the BLS sample, the ultimate torsional moment for NU is larger by 2.3% than the experimental value. Figure 14 shows the crack pattern of a BLS specimen as an example of this group and it shows good agreement for NU result.
Group (4) contains the box girders that were strengthened by CFRP. It consists of three specimens; BLF, BUF and BLUF. The first specimen was strengthened with longitudinal CFRP sheets, the second specimen was strengthened with U-shaped sheets and the third box specimen was strengthened with longitudinal U-shaped sheets. The BLF sample remained in elastic stage until the torsion moment was equivalent to 32 kN.m for EX and 28 kN.m for NU. The sample then entered the phase of plasticity, where it reached an ultimate torsional moment 37.27 kN.m with a rotation angle 0.01429 rad/m for the NU outcomes, and moment 34.95 kN.m with a rotation angle 0.01282 rad/m for EX outcome. The ultimate value of the torsional moment as NU is 6.6 percent larger than the EX value. The BUF sample remained in the elastic phase until the torsion moment became 22.5 kN.m and 25 kN.m as EX and NU results, respectively. After that, the moment increased to be 35.85 kN.m and 38.01 kN.m with corresponding twisting angles of 0.01314 rad/m and 0.00728 rad/m as EX and NU results, respectively. The ultimate value of torsional moment for FEM is less than the experimental by 5.7%. The torsional moment begins to decrease as the angle of rotation increases after reaching the ultimate moment, until the structure collapses. For the BULF sample, the value of the ultimate torsional moment for NU is less than the EX by 6.3%. A good agreement in the NU result of this group was observed as Fig. 14 that contains the crack pattern of a BLUF specimen as an example of this group from both EX and NU outcomes.